136 Chapter 4 / Mathematical Modeling of Fluid Systems and Thermal Systems
ab+b +– Ks
E(s) X(s) Y(s)
Z(s) T
1 s
T 1 T 2 s^2 + (T 1 + 2 T 2 )s+ 1
a
a+b
Figure 4–25
Block diagram for
the system shown in
Figure 4–24.
A block diagram for this system is shown in Figure 4–25. The transfer function
Y(s)/E(s)can be obtained as
Under normal circumstances we design the system such that
then
where
Thus, the controller shown in Figure 4–24 is a proportional-plus-integral-plus-derivative
controller (PID controller).
4–5 Thermal Systems
Thermal systems are those that involve the transfer of heat from one substance to
another. Thermal systems may be analyzed in terms of resistance and capacitance,
although the thermal capacitance and thermal resistance may not be represented
accurately as lumped parameters, since they are usually distributed throughout the sub-
stance. For precise analysis, distributed-parameter models must be used. Here, however,
to simplify the analysis we shall assume that a thermal system can be represented by a
lumped-parameter model, that substances that are characterized by resistance to heat
flow have negligible heat capacitance, and that substances that are characterized by heat
capacitance have negligible resistance to heat flow.
Kp=
b
a
T 1 +2T 2
T 1
, Ki=
b
a
1
T 1
, Kd=
b
a
T 2
=Kp+
Ki
s
+Kd s
Y(s)
E(s)
=
b
a
T 1 T 2 s^2 +AT 1 +2T 2 Bs+ 1
T 1 s
`
a
a+b
K
s
T 1 s
T 1 T 2 s^2 +AT 1 +2T 2 Bs+ 1
` 1
Y(s)
E(s)
=
b
a+b
K
s
1 +
a
a+b
K
s
T 1 s
T 1 T 2 s^2 +AT 1 +2T 2 Bs+ 1
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